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Silicon carbide (SiC) is a wide band gap semiconductor and an attractive candidate for applications in harsh environments such as space, fusion, or future high luminosity colliders. Due to the large band gap, the leakage currents in SiC…

Instrumentation and Detectors · Physics 2023-10-04 Andreas Gsponer , Philipp Gaggl , Jürgen Maier , Richard Thalmeier , Simon Emanuel Waid , Thomas Bergauer

The pixel detector is the innermost tracking device in CMS, reconstructing interaction vertices and charged particle trajectories. The sensors located in the innermost layers of the pixel detector must be upgraded for the ten-fold increase…

The CMS silicon tracker consists of two tracking devices utilizing semiconductor technology: the inner pixel and the outer strip detectors. They operate in a high-occupancy and high-radiation environment presented by particle collisions in…

Instrumentation and Detectors · Physics 2019-08-13 Viktor Veszpremi

Detectors planned for use at the Large Hadron Collider will operate in a radiation field produced by beam collisions. To predict the radiation damage to the components of the detectors, prototype devices are irradiated at test beam…

Instrumentation and Detectors · Physics 2015-06-17 Prabhakar Palni , Martin Hoeferkamp , Aaron Taylor , Sandip Vora , Haley McDuff , Qufei Gu , Sally Seidel

Investigation of HV-CMOS sensors for use as a tracking detector in the ATLAS experiment at the upgraded LHC (HL-LHC) has recently been an active field of research. A potential candidate for a pixel detector built in Silicon-On-Insulator…

Instrumentation and Detectors · Physics 2017-10-27 B. Hiti , V. Cindro , A. Gorišek , T. Hemperek , T. Kishishita , G. Kramberger , H. Krüger , I. Mandić , M. Mikuž , N. Wermes , M. Zavrtanik

Pixel sensors in 3D technology equip the outer ends of the staves of the Insertable B Layer (IBL), the innermost layer of the ATLAS Pixel Detector, which was installed before the start of LHC Run 2 in 2015. 3D pixel sensors are expected to…

Instrumentation and Detectors · Physics 2024-12-18 ATLAS Collaboration

We have exposed seven full length production quality crystals of the electromagnetic calorimeter (ECAL) of the CMS detector to a 20 GeV/c proton beam at the CERN PS accelerator. The exposure was done at fluxes of 10**12 p/cm**2/h and 10**13…

Instrumentation and Detectors · Physics 2017-08-23 M. Huhtinen , P. Lecomte , D. Luckey , F. Nessi-Tedaldi

The high-luminosity LHC (HL-LHC) upgrade is setting now a new challenge for particle detector technologies. The increase in luminosity will produce a particle background in the gas-based muon detectors that is ten times higher than under…

With an expected ten-fold increase in luminosity in S-LHC, the radiation environment in the tracker volumes will be considerably harsher for silicon-based detectors than the already harsh LHC environment. Since 2006, a group of CMS…

Due to the increased commercial availability, wide-bandgap semiconductors and their radiation hardness have recently received increased interest from the particle physics community. 4H-Silicon Carbide (SiC), especially, is an attractive…

Instrumentation and Detectors · Physics 2024-12-11 Andreas Gsponer , Philipp Gaggl , Jürgen Burin , Simon Waid , Thomas Bergauer

The ATLAS collaboration will replace its tracking detector with new all silicon pixel and strip systems. This will allow to cope with the higher radiation and occupancy levels expected after the 5-fold increase in the luminosity of the LHC…

The phase 1 upgrade of the CMS pixel detector has been designed to maintain the tracking performance at instantaneous luminosities of $2 \times 10^{34} \mathrm{~cm}^{-2} \mathrm{~s}^{-1}$. Both barrel and endcap disk systems now feature one…

Instrumentation and Detectors · Physics 2018-07-25 Jory Sonneveld

Signal loss is the main limitation on tracking/vertexing performance due to radiation damage effect to hybrid pixel detectors when irradiated at fluences expected at High Luminosity LHC (HL-LHC). It is important to have reliable predictions…

High Energy Physics - Experiment · Physics 2025-06-13 Marco Bomben

The expected radiation background in the CMS RPC system has been studied using the MC prediction with the CMS FLUKA simulation of the detector and the cavern. The MC geometry used in the analysis describes very accurately the present RPC…

Instrumentation and Detectors · Physics 2020-12-15 R. Hadjiiska , A. Samalan , M. Tytgat , N. Zaganidis , G. A. Alves , F. Marujo , F. Torres Da Silva De Araujo , E. M. Da Costa , D. De Jesus Damiao , H. Nogima , A. Santoro , S. Fonseca De Souza , A. Aleksandrov , P. Iaydjiev , M. Rodozov , M. Shopova , G. Sultanov , M. Bonchev , A. Dimitrov , L. Litov , B. Pavlov , P. Petkov , A. Petrov , S. J. Qian , C. Bernal , A. Cabrera , J. Fraga , A. Sarkar , S. Elsayed , Y. Assran , M. El Sawy , M. A. Mahmoud , Y. Mohammed , C. Combaret , M. Gouzevitch , G. Grenier , I. Laktineh , L. Mirabito , K. Shchablo , I. Bagaturia , D. Lomidze , I. Lomidze , V. Bhatnagar , R. Gupta , P. Kumari , J. Singh , V. Amoozegar , B. Boghrati , M. Ebraimi , R. Ghasemi , M. Mohammadi Najafabadi , E. Zareian , M. Abbrescia , R. Aly , W. Elmetenawee , N. De Filippis , A. Gelmi , G. Iaselli , S. Leszki , F. Loddo , I. Margjeka , G. Pugliese , D. Ramos , M. Caponero , L. Benussi , S. Bianco , S. Colafranceschi , A. Russo , L. Passamonti , D. Piccolo , D. Pierluigi , G. Saviano , S. Buontempo , A. Di Crescenzo , F. Fienga , G. De Lellis , L. Lista , S. Meola , P. Paolucci , A. Braghieri , P. Salvini , P. Montagna , C. Riccardi , P. Vitulo , B. Francois , T. J. Kim , J. Park , S. Y. Choi , B. Hong , K. S. Lee , J. Goh , H. Lee , J. Eysermans , C. Uribe Estrada , I. Pedraza , H. Castilla-Valdez , A. Sanchez-Hernandez , C. A. Mondragon Herrera , D. A. Perez Navarro , G. A. Ayala Sanchez , S. Carrillo , E. Vazquez , A. Radi , A. Ahmad , I. Asghar , H. Hoorani , S. Muhammad , M. A. Shah , I. Crotty

Silicon pixel sensors manufactured using commercial CMOS processes are promising instruments for high-energy particle physics experiments due to their high yield and proven radiation hardness. As one of the essential factors for the…

Instrumentation and Detectors · Physics 2024-04-01 Sinuo Zhang , Ivan Caicedo , Tomasz Hemperek , Toko Hirono , Jochen Dingfelder

The CMS detector at the LHC requires a major upgrade to cope with the higher instantaneous luminosity and the elevated radiation levels. The active media of the forward backing hadron calorimeters is projected to be radiation-hard, high…

Instrumentation and Detectors · Physics 2015-10-30 Emrah Tiras

The High Luminosity LHC (HL-LHC) phase is designed to increase by an order of magnitude the amount of data to be collected by the LHC experiments. The foreseen gradual increase of the instantaneous luminosity of up to more than twice its…

In this paper a detailed simulation of irradiated pixel sensors was used to investigate the effects of radiation damage on the position determination and optimize the hit reconstruction algorithms. The simulation implements a model of…

Instrumentation and Detectors · Physics 2009-11-11 E. Alagoz , V. Chiochia , M. Swartz

The tracking system of the CMS experiment, currently under construction at the Large Hadron Collider (LHC) at CERN (Geneva, Switzerland), will include a silicon pixel detector providing three spacial measurements in its final configuration…

First of its kind, the barrel section of the MIP Timing Detector is a large area timing detector based on LYSO:Ce crystals and SiPMs which are required to operate in an unprecedentedly harsh radiation environment (up to an integrated…

Instrumentation and Detectors · Physics 2025-08-14 F. Addesa , P. Akrap , A. Albert , B. Allmond , T. Anderson , J. Babbar , D. Baranyai , P. Barria , C. Basile , A. Benaglia , A. Benato , M. Benettoni , M. Besancon , N. Bez , S. Bhattacharya , R. Bianco , D. Blend , A. Boletti , A. Bornheim , R. Bugalho , A. Bulla , B. Cardwell , R. Carlin , M. Casarsa , F. Cetorelli , F. Cossutti , B. Cox , G. Da Molin , F. De Guio , K. De Leo , F. De Riggi , P. Debbins , D. Del Re , R. Delli Gatti , J. Dervan , P. Devouge , K. Dreimanis , O. M. Eberlins , F. Errico , E. Fernandez , W. Funk , A. Gaile , M. Gallinaro , R. Gargiulo , R. Gerosa , A. Ghezzi , B. Gyongyosi , Z. Hao , A. H. Heering , Z. Hu , R. Isocrate , M. Jose , A. Karneyeu , M. S. Kim , A. Krishna , B. Kronheim , O. K. Köseyan , A. Ledovskoy , L. Li , Z. Li , V. Lohezic , F. Lombardi , M. T. Lucchini , M. Malberti , Y. Mao , Y. Maravin , B. Marzocchi , D. Mazzaro , R. Menon Raghunandanan , P. Meridiani , C. Munoz Diaz , Y. Musienko , S. Nargelas , L. L. Narváez , C. Neu , G. Organtini , T. Orimoto , D. Osite , M. Paganoni , S. Palluotto , C. Palmer , N. Palmeri , F. Pandolfi , R. Paramatti , T. Pauletto , A. Perego , G. Pikurs , G. Pizzati , R. Plese , C. Quaranta , G. Reales Gutiérrez , N. Redaelli , S. Ronchi , R. Rossin , M. Ö. Sahin , F. Santanastasio , I. Schmidt , D. Sidiropoulos Kontos , T. Sievert , R. Silva , P. Simmerling , L. Soffi , P. Solanki , G. Sorrentino , M. Spiropulu , N. R. Strautnieks , X. Sun , D. D. Szabo , T. Tabarelli de Fatis , G. Tamulaitis , R. Taylor , M. Titov , M. Tosi , G. Trabucco , A. Tsirou , C. Tully , M. Turcato , B. Ujvari , J. Varela , F. Veronese , V. Vladimirov , J. Wang , M. Wayne , S. White , Z. Wu , J. W. Wulff , R. A. Wynne , L. Zhang , M. Zhang , G. Zilizi
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